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PreprintCC BY 4.0arXiv

Dimensionally Regulated Graviton Self-Energy from Gravitons on de Sitter

Abstract

The graviton self-energy −i [μν Σρσ](x;x') is the 1PI 2-point function of quantum gravity. It can be used to quantum-correct the linearized Einstein equation in order to infer quantum corrections to gravitational radiation and to the force of gravity. As long as the two points are non-coincident, the graviton self-energy does not need regularization at 1-loop order, however, solving the 1-loop effective field equations requires integrating [μν Σρσ](x;x') over x'μ, including x'μ = xμ. To facilitate this we employ dimensional regularization and BPHZ renormalization to compute the 1-loop contribution to the graviton self-energy, in pure quantum gravity, on de Sitter background, in the simplest gauge. We then solve the effective field equations to derive 1-loop corrections to the plane wave mode functions of gravitational radiation, and to the Newtonian potential. Although it seems possible to renormalize in such a way that the mode function shows no secular growth, the Newtonian potential grows like the third power of the number of e-foldings.

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BibTeX
@misc{yesilyurt2026dimensionally,
  title = {{Dimensionally Regulated Graviton Self-Energy from Gravitons on de Sitter}},
  author = {B. Yesilyurt and N. C. Tsamis and R. P. Woodard},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.02120},
  eprint = {2611.02120},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.02120},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Dimensionally Regulated Graviton Self-Energy from Gravitons on de Sitter
AU  - B. Yesilyurt
AU  - N. C. Tsamis
AU  - R. P. Woodard
PY  - 2026
DA  - 2026/11/01
PB  - arXiv
DO  - 10.48550/arxiv.2611.02120
UR  - https://arxiv.org/abs/2611.02120
AB  - The graviton self-energy −i [^μν Σ^ρσ](x;x') is the 1PI 2-point function of quantum gravity. It can be used to quantum-correct the linearized Einstein equation in order to infer quantum corrections to gravitational radiation and to the force of gravity. As long as the two points are non-coincident, the graviton self-energy does not need regularization at 1-loop order, however, solving the 1-loop effective field equations requires integrating [^μν Σ^ρσ](x;x') over x'^μ, including x'^μ = x^μ. To facilitate this we employ dimensional regularization and BPHZ renormalization to compute the 1-loop contribution to the graviton self-energy, in pure quantum gravity, on de Sitter background, in the simplest gauge. We then solve the effective field equations to derive 1-loop corrections to the plane wave mode functions of gravitational radiation, and to the Newtonian potential. Although it seems possible to renormalize in such a way that the mode function shows no secular growth, the Newtonian potential grows like the third power of the number of e-foldings.
ER  -